Derive a finite phasor sum and remove its singularities
For N equally illuminated narrow slits, adjacent paths differ by q wavelengths and adjacent phases by 2πq. The total field in single-slit units is A=Σ from j=0 to N−1 exp(i2πjq). This finite sum is always defined, including when every phasor points in the same direction.
Learning outcome: Sum real and imaginary components directly, compare with the geometric ratio away from its removable singularities and integrate a full q period to check the power scaling.
Starting recap
Retain complex amplitude before intensity, definite-integral boundaries, normalization, calibration covariance and unused evidence.
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For N=4 and q=0.25, the phasors are 1,i,−1,−i and sum to zero. At q=0 the field is 4 and intensity 16. The nearest zero is 0.25 away in q, and period-averaged intensity is 4.
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How can peak intensity grow quadratically while period-averaged intensity grows linearly?
Experiment
Sum real and imaginary components directly, compare with the geometric ratio away from its removable singularities and integrate a full q period to check the power scaling.
Sum a finite array without a singular ratio
Worked teaching model · synthetic values · Original equally illuminated narrow-slit array. Sum N unit complex amplitudes with adjacent phase 2πq. The geometric ratio has removable singularities at integer q; direct finite sums retain principal maxima. Finite slit envelope and imperfect coherence are omitted.
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Finite phasor summation remains defined at principal maxima; increasing N narrows peaks without changing their spacing in q.
Original equally illuminated narrow-slit array. Sum N unit complex amplitudes with adjacent phase 2πq. The geometric ratio has removable singularities at integer q; direct finite sums retain principal maxima. Finite slit envelope and imperfect coherence are omitted.
The vertical axis is rescaled to this case’s actual range; equal display height does not imply equal optical power. The finite curve is illustrative; the ledger preserves the exact case values and stated numerical quadrature.
| Quantity | Value | Unit |
|---|---|---|
| Real summed field | -1.83697e-16 | single-slit amplitudes |
| Imaginary summed field | 2.22045e-16 | single-slit amplitudes |
| Intensity relative to one slit | 8.30484e-32 | ratio |
| Intensity relative to principal maximum | 5.19053e-33 | ratio |
| Principal maximum relative to one slit | 16 | ratio |
| Nearest-zero displacement in q | 0.250000 | ratio |
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Finite phasor summation remains defined at principal maxima; increasing N narrows peaks without changing their spacing in q.
Original equally illuminated narrow-slit array. Sum N unit complex amplitudes with adjacent phase 2πq. The geometric ratio has removable singularities at integer q; direct finite sums retain principal maxima. Finite slit envelope and imperfect coherence are omitted.
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Use N=6 and q=0.5, then compare the nearest-zero distance with N=2.
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